Lei Chen (LChen95@umd.edu) University of Maryland, College Park Sept. 2020 This file contains the dataset for “Perfect Absorption in Complex Scattering Systems with or without Hidden Symmetries” by Lei Chen, Tsampikos Kottos, and Steven M. Anlage. Funding acknowledgements: This work is supported by the AFOSR under COE Grant FA9550-15-10171, the ONR under Grants N000141912481 and N00014-19-1-2480, and the Maryland Quantum Materials Center. Data list: - Figure 2a: S-matrix "zero-crossing" eigenvalues trajectories in the experiment. Examples of six frequencies are listed. For each frequency, the first column is the real part of the eigenvalue, and the second column is the imaginary part of the eigenvalue. - Figure 2b: S-matrix "zero-crossing" eigenvalues trajectories in the simulation. Examples of six frequencies are listed. For each frequency, the first column is the real part of the eigenvalue, and the second column is the imaginary part of the eigenvalue. - Figure 3a: Frequency sweep measurement data for the CPA state. P_out / P_in = (P_out from Port 1 + P_out from Port 2)/(P_in from Port 1 + P_in from Port 2) - Figure 3b: Attenuation sweep measurement data for the CPA state. P_out / P_in = (P_out from Port 1 + P_out from Port 2)/(P_in from Port 1 + P_in from Port 2) - Figure 3c: Amplitude sweep measurement data for the CPA state. P_out / P_in = (P_out from Port 1 + P_out from Port 2)/(P_in from Port 1 + P_in from Port 2) - Figure 3d: Phase sweep measurement data for the CPA state. P_out / P_in = (P_out from Port 1 + P_out from Port 2)/(P_in from Port 1 + P_in from Port 2) - Figure 4: Voltage profile and power distribution of CPA state in idealized simulation. - Figure 5: Frequency sweep measurement data for two CPA states in the 2D bow-tie billiard under two different input waveforms. P_out / P_in = (P_out from Port 1 + P_out from Port 2)/(P_in from Port 1 + P_in from Port 2) - Figure 6a: Frequency sweep measurement data for the CPA state in the complex network with Broken Time-reversal invariance. P_out / P_in = (P_out from Port 1 + P_out from Port 2)/(P_in from Port 1 + P_in from Port 2) - Figure 6b: Attenuation sweep measurement data for the CPA state in the complex network with Broken Time-reversal invariance. P_out / P_in = (P_out from Port 1 + P_out from Port 2)/(P_in from Port 1 + P_in from Port 2) - Figure 6c: Amplitude sweep measurement data for the CPA state in the complex network with Broken Time-reversal invariance. P_out / P_in = (P_out from Port 1 + P_out from Port 2)/(P_in from Port 1 + P_in from Port 2) - Figure 6d: Phase sweep measurement data for the CPA state in the complex network with Broken Time-reversal invariance. P_out / P_in = (P_out from Port 1 + P_out from Port 2)/(P_in from Port 1 + P_in from Port 2) - Supplementary Figure 2: Voltage profile and power distribution of "Anti-CPA" state in idealized simulation. - Supplementary Figure 3: det(S) from experiment and simulation. - Supplementary Figure 4a: Amplitude sweep measurement data for the CPA state in the 2D bow-tie billiard. P_out / P_in = (P_out from Port 1 + P_out from Port 2)/(P_in from Port 1 + P_in from Port 2) - Supplementary Figure 4b: Phase sweep measurement data for the CPA state in the 2D bow-tie billiard. P_out / P_in = (P_out from Port 1 + P_out from Port 2)/(P_in from Port 1 + P_in from Port 2)